Lipid bilayer mechanics in a pipette with glass-bilayer adhesion

Electrophysiology is a central tool for measuring how different driving forces (e.g., ligand concentration, transmembrane voltage, or lateral tension) cause a channel protein to gate. Upon formation of the high resistance seal between a lipid bilayer and a glass pipette, the so-called “giga-seal”, channel activity can be recorded electrically. In this article, we explore the implications of giga-seal formation on the mechanical state of a lipid bilayer patch. We use a mechanical model for the free energy of bilayer geometry in the presence of glass-bilayer adhesion to draw three potentially important conclusions. First, we use our adhesion model to derive an explicit relationship between applied pressure and patch shape that is consistent with the Laplace-Young Law, giving an alternative method of calculating patch tension under pressure. With knowledge of the adhesion constant, which we find to be in the range ∼0.4–4 mN/m, and the pipette size, one can precisely calculate the patch tension as a function of pressure, without the difficultly of obtaining an optical measurement of the bilayer radius of curvature. Second, we use data from previous electrophysiological experiments to show that over a wide range of lipids, the resting tension on a electrophysiological patch is highly variable and can be 10–100 times higher than estimates of the tension in a typical cell membrane. This suggests that electrophysiological experiments may be systematically altering channel-gating characteristics and querying the channels under conditions that are not the same as their physiological counterparts. Third, we show that reversible adhesion leads to a predictable change in the population response of gating channels in a bilayer patch.     

Cell membrane patches are supported by proteoglycans

A cell membrane patch isolated on a patch clamp pipette incorporates in addition to the phospholipid bilayer, an extracellular matrix and cytoskeletal components. The significance of the extracellular matrix for the patch formation was studied in aortic smooth muscle and cerebellar granule cells grow in the presence of an inhibitor of proteoglycan synthesis, -d -xyloside. The xyloside improved the seal success rate, and after patch excision membrane vesicles were formed instead of inside-out patches. When amphotericin B was included in the pipette solution, perforated outside-out vesicles were formed in 96% of cells. The findings suggest, that membrane patches are supported by the extracellular matrix or by structures that relate to this matrix.     

Adaptive behavior of bacterial mechanosensitive channels is coupled to membrane mechanics

Mechanosensitive channel of small conductance (MscS), a tension-driven osmolyte release valve residing in the inner membrane of Escherichia coli, exhibits a complex adaptive behavior, whereas its functional counterpart, mechanosensitive channel of large conductance (MscL), was generally considered nonadaptive. In this study, we show that both channels exhibit similar adaptation in excised patches, a process that is completely separable from inactivation prominent only in MscS. When a membrane patch is held under constant pressure, adaptation of both channels is manifested as a reversible current decline. Their dose–response curves recorded with 1–10-s ramps of pressure are shifted toward higher tension relative to the curves measured with series of pulses, indicating decreased tension sensitivity. Prolonged exposure of excised patches to subthreshold tensions further shifts activation curves for both MscS and MscL toward higher tension with similar magnitude and time course. Whole spheroplast MscS recordings performed with simultaneous imaging reveal activation curves with a midpoint tension of 7.8 mN/m and the slope corresponding to ∼15-nm² in-plane expansion. Inactivation was retained in whole spheroplast mode, but no adaptation was observed. Similarly, whole spheroplast recordings of MscL (V23T mutant) indicated no adaptation, which was present in excised patches. MscS activities tried in spheroplast-attached mode showed no adaptation when the spheroplasts were intact, but permeabilized spheroplasts showed delayed adaptation, suggesting that the presence of membrane breaks or edges causes adaptation. We interpret this in the framework of the mechanics of the bilayer couple linking adaptation of channels in excised patches to the relaxation of the inner leaflet that is not in contact with the glass pipette. Relaxation of one leaflet results in asymmetric redistribution of tension in the bilayer that is less favorable for channel opening.     

Membrane tension regulates water transport in yeast

Evidence that membrane surface tension regulates water fluxes in intact cells of a Saccharomyces cerevisiae strain overexpressing aquaporin AQY1 was obtained by assessing the osmotic water transport parameters in cells equilibrated in different osmolarities. The osmotic water permeability coefficients (P_f) obtained for yeast cells overexpressing AQY1 incubated in low osmolarity buffers were similar to those obtained for a double mutant aqy1aqy2 and approximately three times lower (with higher activation energy, E_a) than values obtained for cells incubated in higher osmolarities (with lower E_a). Moreover, the initial inner volumes attained a maximum value for cells equilibrated in lower osmolarities (below 0.75 M) suggesting a pre-swollen state with the membrane under tension, independent of aquaporin expression. In this situation, the impairment of water channel activity suggested by lower P_f and higher E_a could probably be the first available volume regulatory tool that, in cooperation with other osmosensitive solute transporters, aims to maintain cell volume. The results presented point to the regulation of yeast water channels by membrane tension, as previously described in other cell systems.     

Diversity of K+ channels in the basolateral membrane of restingnecturus oxyntic cells

Summary Patch-clamp techniques have been applied to characterize the channels in the basolateral membrane of resting (cimetidine-treated, nonacid secreting) oxyntic cells isolated from the gastric mucosa ofNecturus maculosa. In cell-attached patches with pipette solution containing 100mm KCl, four major classes of K⁺ channels can be distinguished on the basis of their kinetic behavior and conductance: (1) 40% of the patches contained either voltage-independent (a) or hyperpolarization-activated (b), inward-rectifying channels with short mean open times (16 msec fora, and 8 msec forb). Some channels showed subconductance levels. The maximal inward conductanceg _max was 31±5 pS (n=13) and the reversal potentialE _rev was atV _p=–34±6 mV (n=9). (2) 10% of the patches contained depolarization-activated and inward-rectifying channels withg _max=40 ±18 pS (n=3) andE _rev was atV _p=–31±5 mV (n=3). With hyperpolarization, the channels open in bursts with rapid flickerings within bursts. Addition of carbachol (1mm) to the bath solution in cell-attached patches increased the open probabilityP _o of these channels. (3) 10% of the patches contained voltage-independent inward-rectifying channels withg _max=21±3 pS (n=4) andE _rev was atV _p=–24±9 mV (n=4). These channels exhibited very high open probability (P _o=0.9) and long mean open time (1.6 sec) at the resting potential. (4) 20% of the patches contained voltage-independent channels with limiting inward conductance of 26±2 pS (n=3) andE _rev atV _p=–33±3 mV (n=3). The channels opened in bursts consisting of sequential activation of multiple channels with very brief mean open times (10 msec). In addition, channels with conductances less than 6 pS were observed in 20% of the patches. In all nine experiments with K⁺ in the pipette solution replaced by Na⁺, unitary currents were outward, and inward currents were observed only for large hyperpolarizing potentials. This indicates that the channels are more selective for K⁺ over Na⁺ and Cl^–. A variety of K⁺ channels contributes to the basolateral K⁺ conductance of resting oxyntic cells.     

Quantitative video microscopy of patch clamped membranes stress, strain, capacitance, and stretch channel activation.

Membrane patches from chick skeletal muscle were stretched by applying controlled suction or pressure to the pipette. From images of the patch, the patch dimensions (area and radius of curvature) were computed by nonlinear regression of the images to a geometric model. With no applied pressure, patch membranes are nearly planar and normal to the wall of the pipette. With increasing pressure gradients, the patch bulges, the radius of curvature decreases, and the area increases. The patch capacitance changes in exact proportion to the change in area at a rate of 0.7 microF/cm2. The increase in area is due to a flow of lipid (with perhaps small amounts of diffusible protein) along the walls of the pipette into the patch. The flow is reversible with a relaxation of the pressure gradient. The area elastic constant of the membrane is approximately 50 dyn/cm, insensitive to cytochalasin B and probably represents the elasticity of the underlying spectrin/dystrophin network. Simultaneous measurements of stretch activated (SA) ion channel activity in the patch showed that the sensitivity of channels from different patches, although different when calculated as a function of applied pressure, was the same when calculated as a function of tension. Because patch lipid is free to flow, and hence stress-free in the steady state, SA channels must be activated by tension in the cytoskeleton.     

Stretch-activated chloride,potassium, and calcium channels coexisting in plasma membranes of guard cells of Vicia faba L.

Mechanosensitive ion channels in the plasma membrane of Vicia faba guard cell protoplasts were studied by use of the patch clamp technique. Stretch-activated (SA) channels in outside-out patches were analyzed for channel conductance, kinetics and ion selectivity. We found three distinct SA channels, permeable to Cl^–, K⁺ and Ca²⁺ and distinguishable from spontaneous (non-SA) channels for these ions on the basis of conductance, kinetics, and voltage-dependence, as well as sensitivity to membrane stretch. In the attached patch configuration, light suction (2 to 10 kPa) reversibly induced channel opening with multiple amplitudes and complex kinetics. The open probability for SA channels increased nonlinearly with pipette suction. In guard cells in situ, these SA channels may mediate ion transport across the plasma membrane directly, as well as influence the activity of non-SA channels via effects on membrane voltage and cytoplasmic calcium. Through such effects, SA channels likely influence volume and turgor regulation of guard cells, and thereby control of leaf gas exchange.Abbreviations EK equilibrium potential for potassium transport - E_Cl equilibrium potential for chloride transport - SA stretchactivated Dedicated to the 80. birthday of Franz HedrichSupported by a grant from the Deutsche Forschungsgemeinschaft to R.H. and a Department of Energy grant to D.J.C. gratefully acknowledges a John S. Guggenheim Fellowship and Fulbright Kommission Senior Professor Award. We thank Ingrid Baumann and Angela Schön for technical assistance, and Klaus Raschke and Heiner Busch for spirited discussions and support.     

CFTR Channels Expressed in CHO Cells Do Not Have Detectable ATP Conductance

The cystic fibrosis transmembrane conductance regulator (CFTR) is a cAMP-activated, ATP-dependent chloride channel which may have additional functions. Recent reports that CFTR mediates substantial electrodiffusion of ATP from epithelial cells have led to the proposal that CFTR regulates other ion channels through an autocrine mechanism involving ATP. The aim of this study was to determine the ATP conductance of wild-type CFTR channels stably expressed in Chinese hamster ovary cells using patch clamp techniques. In the cell-attached configuration with 100 mm Mg · ATP or Tris · ATP solution in the pipette and 140 mm NaCl in the bath, exposing cells to forskolin caused the activation of a low-conductance channel having kinetics resembling those of CFTR. Single channel currents were negative at the resting membrane potential (V _m ), consistent with net diffusion of Cl from the cell into the pipette. The transitions decreased in amplitude, but did not reverse direction, as V _m was clamped at increasingly positive potentials to enhance the driving force for inward ATP flow (>+80 mV). In excised patches, single channel currents did not reverse under essentially biionic conditions (Cl_in/ATP_out or ATP_in/Cl_out), although PKA-activated currents were clearly visible in the same patches at voltages where they would be carried by chloride ions. Moreover, with NaCl solution in the bath and a mixture of ATP and Cl in the pipette, the single channel I/V curve reversed at the predicted equilibrium potential for chloride. CFTR channel currents disappeared when patches were exposed to symmetrical ATP solutions and were restored by reexposure to Cl solution. Finally, in the whole-cell configuration with NaCl in the bath and 100 mm MgATP or TrisATP in the pipette, cAMP-stimulated cells had time-independent, outwardly rectifying currents consistent with CFTR selectivity for external Cl over internal ATP. Whole-cell currents reversed near V _m =−55 mV under these conditions, however the whole cell resistance measured at −100 mV was comparable to that of the gigaohm seal between the plasma membrane and glass pipette (7 GΩ). We conclude that CFTR does not mediate detectable electrodiffusion of ATP. Received: 8 November 1995/Revised: 23 January 1996     

Mitochondria Present in Excised Patches From Pancreatic B-cells May Form Microcompartments With ATP-Dependent Potassium Channels

Experiments with inside-out patches excised from pancreatic B-cells have yielded evidence that mitochondria are often contained in the cytoplasmic plug protruding into the tip of patch pipette. When intact B-cells were loaded with the fluorescent mitochondrial stain, rhodamine 123, and membrane patches excised from these cells, a green fluorescence could be observed in the lumen at the tip of the patch pipette. The same result was obtained with the mitochondrial stain, MitoTracker Green FM, which is only fluorescent in a membrane-bound state. Furthermore, the open probability of ATP-dependent potassium (K_ATP) channels in inside-out patches was influenced by mitochondrial fuels and inhibitors. Respiratory substrates like tetramethyl phenylene diamine (2 mM) plus ascorbate (5 mM) or -ketoisocaproic acid (10 mM) reduced the open probability of K_ATP channels in inside-out patches significantly (down to 57% or 65% of control, respectively). This effect was antagonized by the inhibitor of cytochrome oxidase, sodium azide (5 mM). Likewise, the inhibitor of succinate dehydrogenase, malonate (5 mM), increased the open probability of K_ATP channels in the presence of succinate (1 mM). However, oligomycin in combination with antimycin and rotenone did not increase open probability. Although it cannot be excluded that these effects result from a direct interaction with the K_ATP channels, the presence of mitochondria in the close vicinity permits the hypothesis that changes in mitochondrial metabolism are involved, mitochondria and K_ATP channels thus forming functional microcompartments.     

Chloride channels in human platelets: Evidence for activation by internal calcium

Summary Whole-cell patch-clamp recordings were made from freshly isolated human platelets. The pipette contained a high concentration of divalent cations, which permitted easy disruption of cell-attached membrane patches by suction. Single-channel currents were measured when the pipette contained isotonic BaCl₂ or MgCl₂ saline; over 30 sec –5 min an increasing number of channels appeared until conductance steps through individual channels could no longer be distinguished. The current-voltage relationship was curvilinear; chord conductance at –35 mV was 25 pS increasing to 45 to 52 pS at +45 mV. Ion substitution experiments showed the current to be primarily carried by Cl^–.E _rev was shifted 30 mV/10-fold change in external Cl^– (replaced by gluconate), was similar with BaCl₂ or MgCl₂ in the pipette and was not significantly shifted by replacing external Na⁺ with K⁺. Addition of 1mm BAPTA to the MgCl₂ pipette saline prevented activation of Cl^– currents; with isotonic CaCl₂ internal saline, current appeared immediately upon patch rupture, suggesting that the Cl^– channels are dependent on internal Ca²⁺, 5-nitro-2-(3-phenylpropylamino)-benzoate, reported to block a Cl^– conductance in studies of rat epithelial cells, caused a potent flickery block and may be a useful tool with which to investigate the physiological role of Cl^– currents in human platelets.     

The structure and dynamics of patch-clamped membranes: a study using differential interference contrast light microscopy

We have developed techniques for micromanipulation under high power video microscopy. We have used these to study the structure and motion of patch-clamped membranes when driven by pressure steps. Patch-clamped membranes do not consist of just a membrane, but rather a plug of membrane-covered cytoplasm. There are organelles and vesicles within the cytoplasm in the pipette tip of both cell-attached and excised patches. The cytoplasm is capable of active contraction normal to the plane of the membrane. With suction applied before seal formation, vesicles may be swept from the cell surface by shear stress generated from the flow of saline over the cell surface. In this case, patch recordings are made from membrane that was not originally present under the tip. The vesicles may break, or fuse and break, to form the gigasealed patch. Patch membranes adhere strongly to the wall of the pipette so that at zero transmural pressure the membranes tend to be normal to the wall. With transmural pressure gradients, the membranes generally become spherical; the radius of curvature decreasing with increasing pressure. Some patches have nonuniform curvature demonstrating that forces normal to the membrane may be significant. Membranes often do not respond quickly to changes in pipette pressure, probably because viscoelastic cytoplasm reduces the rate of flow through the tip of the pipette. Inside-out patches may be peeled from the walls of the pipette, and even everted (with positive pressure), without losing the seal. This suggests that the gigaseal is a distributed property of the membrane-glass interface.     

Geometrical Membrane Curvature as an Allosteric Regulator of Membrane Protein Structure and Function

Transmembrane proteins are embedded in cellular membranes of varied lipid composition and geometrical curvature. Here, we studied for the first time the allosteric effect of geometrical membrane curvature on transmembrane protein structure and function. We used single-channel optical analysis of the prototypic transmembrane β-barrel α-hemolysin (α-HL) reconstituted on immobilized single small unilamellar liposomes of different diameter and therefore curvature. Our data demonstrate that physiologically abundant geometrical membrane curvatures can enforce a dramatic allosteric regulation (1000-fold inhibition) of α-HL permeability. High membrane curvatures (1/diameter ∼1/40 nm⁻¹) compressed the effective pore diameter of α-HL from 14.2 ± 0.8 Å to 11.4 ± 0.6 Å. This reduction in effective pore area (∼40%) when combined with the area compressibility of α-HL revealed an effective membrane tension of ∼50 mN/m and a curvature-imposed protein deformation energy of ∼7 k_BT. Such substantial energies have been shown to conformationally activate, or unfold, β-barrel and α-helical transmembrane proteins, suggesting that membrane curvature could likely regulate allosterically the structure and function of transmembrane proteins in general.     

Single Mechanosensitive and Ca2+-Sensitive Channel Currents Recorded from Mouse and Human Embryonic Stem Cells

Cell-attached and inside-out patch clamp recording was used to compare the functional expression of membrane ion channels in mouse and human embryonic stem cells (ESCs). Both ESCs express mechanosensitive Ca²⁺ permeant cation channels (MscCa) and large conductance (200 pS) Ca²⁺-sensitive K⁺ (BK_Ca2+) channels but with markedly different patch densities. MscCa is expressed at higher density in mESCs compared with hESCs (70 % vs. 3 % of patches), whereas the BK_Ca2+ channel is more highly expressed in hESCs compared with mESCs (~50 % vs. 1 % of patches). ESCs of both species express a smaller conductance (25 pS) nonselective cation channel that is activated upon inside-out patch formation but is neither mechanosensitive nor strictly Ca²⁺-dependent. The finding that mouse and human ESCs express different channels that sense membrane tension and intracellular [Ca²⁺] may contribute to their different patterns of growth and differentiation in response to mechanical and chemical cues.     

Ion fluxes in giant excised cardiac membrane patches detected and quantified with ion-selective microelectrodes

We have used ion-selective electrodes (ISEs) to quantify ion fluxes across giant membrane patches by measuring and simulating ion gradients on both membrane sides. Experimental conditions are selected with low concentrations of the ions detected on the membrane side being monitored. For detection from the cytoplasmic (bath) side, the patch pipette is oscillated laterally in front of an ISE. For detection on the extracellular (pipette) side, ISEs are fabricated from flexible quartz capillary tubing (tip diameters, 2-3 microns), and an ISE is positioned carefully within the patch pipette with the tip at a controlled distance from the mouth of the patch pipette. Transport activity is then manipulated by solution changes on the cytoplasmic side. Ion fluxes can be quantified by simulating the ion gradients with appropriate diffusion models. For extracellular (intrapatch pipette) recordings, ion diffusion coefficients can be determined from the time courses of concentration changes. The sensitivity and utility of the methods are demonstrated with cardiac membrane patches by measuring (a) potassium fluxes via ion channels, valinomycin, and Na/K pumps; (b) calcium fluxes mediated by Na/Ca exchangers; (c) sodium fluxes mediated by gramicidin and Na/K pumps; and (d) proton fluxes mediated by an unknown electrogenic mechanism. The potassium flux-to-current ratio for the Na/K pump is approximately twice that determined for potassium channels and valinomycin, as expected for a 3Na/2K pump stoichiometery (i.e., 2K/charge moved). For valinomycin-mediated potassium currents and gramicidin-mediated sodium currents, the ion fluxes calculated from diffusion models are typically 10-15% smaller than expected from the membrane currents. As presently implemented, the ISE methods allow reliable detection of calcium and proton fluxes equivalent to monovalent cation currents <1 pA in magnitude, and they allow detection of sodium and potassium fluxes equivalent to <5 pA currents. The capability to monitor ion fluxes, independent of membrane currents, should facilitate studies of both electrogenic and electroneutral ion-coupled transporters in giant patches.     

Extinction times for closed epidemics: the effects of host spatial structure

Although of practical importance, the relationship between the duration of an epidemic and host spatial structure is poorly understood. Here we use a stochastic metapopulation model for the transmission of infection in a spatially structured host population. There are three qualitatively different regimes for the extinction time, which depend on patch population size, the within‐patch basic reproductive number and the strength of coupling between patches. In the first regime, the extinction time for the metapopulation (i.e. from all patches) is approximately equal to the extinction time for a single patch. In the second regime, the metapopulation extinction time is maximal but also highly variable. In the third regime, the extinction time for the metapopulation (T_E) is given by T_E = a + bn^1/2 where a is the local extinction time (i.e. from last patch), b is the transit time (i.e. the time taken for infection to spread from one patch to another) and n is the total number of patches.     

Gated, ion-selective channels observed with patch pipettes in the absence of membranes: novel properties of a gigaseal.

Gigaohm seals made between patch pipettes and hydrophobic substrates have a finite conductance which are cation-selective and capable of producing quantized gating indistinguishable from the gating of biological ion channels. The selectivity sequence and streaming potentials of these seals suggests the existence of a pore of similar dimensions to the nicotinic acetylcholine channel. The ionic selectivity of these seals appears similar to the seal selectivity observed with membrane patches (Fischmeister, R., R. K. Ayer, and R. L. DeHann. 1986. Pfluegers Arch. 406:73-82) and the possibility of discrete gating within the seal region suggests caution when interpreting patch clamp data from unfamiliar preparations. The data suggests that the permeation pathway is the narrow space between the hydrophobic substrate and the pipette. Since this space has one hydrophobic wall, a hydrophilic channel lining may not be essential for channel permeation and gating.     

Identification of Anion-selective Channels in the Basolateral Membrane of Mitochondria-rich Epithelial Cells

Epithelial cells of toad (Bufo bufo) skin were isolated by treatments of the epidermis with collagenase and trypsin. Cl^- channels in the basolateral membrane from soma or neck of mitochondria-rich cells were studied in cell-attached and excised inside-out configurations. Of a total of 87 sealed patches only 28 (32%) were electrically active, and in these we identified four different types of Cl^- channels. The two major populations constituted Ohmic Cl^- channels with limiting conductance (γ_125/125) of 10 pS and 30 pS, respectively. A much rarer 150 pS Ohmic Cl^- channel was also characterized. From i/V relationships of individual channels the following Goldman-Hodgkin-Katz permeabilities were calculated, 2.2 (±0.1) × 10^-14, 5.7 (±0.7) × 10^-14, and 32 (±2) × 10^-14 cm³/sec, for the 10, 30 and 150 pS Cl^- channels, respectively. The 30 pS channel was activated by hyperpolarization. The gating kinetics of the 150 pS channel was complex with burstlike closures within openings of long duration. The fourth type of Cl^- channel was studied in patches generating `noisy currents' with no discrete single-channel events, but with vanishing fluctuations at pipette potentials near E _Cl. Noise analysis revealed a power spectrum with cutoff frequencies of 1.2 and 13 Hz, indicating that resolution of kinetic steps was limited by small channel currents rather than fast channel gating. From the background noise level we estimated the channel conductance to be less than 1.7 pS. Despite the fact that the majority of patches did not contain electrically active Cl^- channels, patches being active, generally, contained more than a single active channel. Thus, for the above three types of resolvable channels, the mean number of active channels per patch amounted to 2.1, 1.4, and 2.0, respectively. This observation, like the finding of few patches with several unresolvable channels, indicates that electrically active Cl^- channels are organized in clusters. Received: 10 October 1996/Revised: 8 January 1997     

Ion channels in Arabidopsis plasma membrane : transport characteristics and involvement in light-induced voltage changes

White light (25 watts per square meter) induced an increase in plasma membrane K⁺-channel activity and a 30- to 70-millivolt transient membrane depolarization (completed in 2-3 minutes) in Arabidopsis thaliana leaf mesophyll cells. Transport characteristics of three types of ion channels in the plasma membrane were determined using inside-out patches. With 220 millimolar K⁺ on the cytoplasmic side of the patch and 50 millimolar K⁺ in the pipette, (220/50 K), the open-channel current-voltage curves of these channels were sigmoidal and consistent with an enzyme kinetic model. Two channel types were selective for K⁺ over Na⁺ and Cl⁻. One (named PKC1) had a maximum conductance (G_max) of 44 picosiemens at a membrane voltage (V_m) of −65 mV in (220/50 K) and is stimulated by light. The other (PKC2) had G_max = 66 picosiemens at V_m = 60 millivolts in (220/50 K). The third channel type (PCC1) transported K⁺ and Na⁺ about equally well but not Cl⁻. It had G_max = 109 picosiemens at V_m = 55 millivolts in (250/50 K) with 10 millimolar Ca²⁺ on the cytoplasmic side. Reducing Ca²⁺ to 0.1 millimolar increased PCC1 open-channel currents by approximately 50% in a voltage-independent manner. Averaged over time, PKC2 and PCC1 currents strongly outward rectified and PKC1 currents did so weakly. Reductants (1 millimolar dithiothreitol or 10 millimolar β-mercaptoethanol) added to the cytoplasmic side of an excised patch increased the open probability of all three channel types.     

Channels activated by stretch in neurons of a helix snail.

Single-channel recordings from central neurons of the helix snail, Cepaea nemoralis, revealed two types of channels that could be activated by stretch (i.e., by the membrane deformation produced when suction is applied to the patch pipette). One, a K+ channel (58 pS in physiological solution), was evident in excised and cell-attached patches. Its conductance in symmetrical [K+] solutions indicated a channel of high K+ permeability (PK = 3.4 x 10(-13) cm/s). Though osmoregulation has been suggested as a function for such channels, comparisons among molluscs indicate osmotic milieu does not govern their expression; Cepaea is terrestrial, and stretch-activated K+ channels similar to those described here occur in aquatic and marine molluscs. The second type of channel, observed only in excised patches, was Cl- permeant; it had a large conductance (130 pS) and was inactive prior to patch excision. Membrane tension may not be the physiological activator of either the K+ or Cl- channel; the channels are designated as stretch-activated channels on the basis of their experimental behaviour during single-channel recording.     

DIDS increases K+ secretion through an I sKchannel in apical membrane of vestibular dark cell epithelium of gerbil

Vestibular dark cell epithelium secretes K⁺ via I _sKchannels in the apical membrane. The previous observation that disulfonic stilbenes increased the equivalent short circuit current (I _sc) suggested that these agents might be useful investigative tools in this tissue. The present experiments were conducted to determine if the increase in I _scwas associated with an increase in K⁺ flux and if the effect was directly on the I _sKchannel or indirectly via a cytosolic intermediary. Measurements of transepithelial K⁺ flux with the K⁺-selective vibrating probe and of changes in net cellular solute flux by measurements of epithelial cell height showed that 4,4-diisothiocyanatostilbene-2,2-disulfonic acid (DIDS) increased K⁺ flux by a factor of 1.96±0.71 and caused net solute efflux. The apical membrane was partitioned with a macropatch pipette and DIDS was applied either to the membrane outside the pipette, inside the pipette or to the entire apical membrane. DIDS inside the pipette increased the current across the patch, the membrane conductance, the slowly-inactivating (I _sK) component of the membrane current and shifted the reversal voltage toward the equilibrium potential for K⁺. DIDS outside the patch decreased the patch current and conductance, consistent with shunting of current away from the membrane patch. These findings strongly support the notion that DIDS increases K⁺ secretion through I _sKchannels in the apical membrane of vestibular dark cell epithelium by acting directly on the channels or on a tightly colocalized membrane component.We thank Dr. Peter J.S. Smith and Alan Shipley of the National Vibrating Probe Facility at the Marine Biological Laboratory at Woods Hole, MA for their support and assistance in the measurements of K⁺ flux. This work was supported by National Institutes of Health grants R01-DC00212, R29-DC1098 and P41-RR01395.